Vector Mechanics For Engineers
Vector Mechanics For Engineers
12th Edition
ISBN: 9781259977305
Author: BEER, Ferdinand P. (ferdinand Pierre), Johnston, E. Russell (elwood Russell), Cornwell, Phillip J., SELF, Brian P.
Publisher: Mcgraw-hill Education,
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Chapter 13, Problem 13.201RP

The 2-Ib ball at A is suspended by an inextensible cord and given an initial horizontal velocity of v0 , If l = 2 ft, v 0 = 0.3 ft, and y B = 0.4 ft, determine the initial velocity v0 so that the ball will enter the basket. (Hint: Use a computer to solve the resulting set of equations.)

Chapter 13, Problem 13.201RP, The 2-Ib ball at A is suspended by an inextensible cord and given an initial horizontal velocity of

Expert Solution & Answer
Check Mark
To determine

The initial velocity v0

Answer to Problem 13.201RP

Initial velocity v0

v0=15.35ft/s.

Explanation of Solution

Given information:

Vector Mechanics For Engineers, Chapter 13, Problem 13.201RP

Weight of ball is 2lb

l=2ft

xB=0.3ft

yB=0.4ft

The principle of conservation of energy is defined as,

When a particle moves under the action of conservation of forces, the sum of kinetic energy and potential energy of that particle remains constant.

T1+V1=T2+V2

Calculation:

At position 1,

v1=v0

At position 2,

The tension Q is equal to zero

F=0

Q+mgsinθ=man=mv22l

Therefore,

v2=glsinθ

According to conservation of energy,

T1+V1=T2+V2

Therefore,

12mv02mgl=12mv22+mglsinθv02=v22+2gl(1+sinθ)

At position 2,

x2= cosθy2=  sinθ

Assume t2 be the time when the ball is in position 2,

For horizontal motion,

x˙=v2sinθx =x2(v2sinθ)(tt2)

At point B,

x=xB   t=tB

Therefore,

(tBt2)=lcosθxBv2sinθ

For vertical motion,

y˙=v2cosθg(tt2)

y=y2+(v2cosθ)(tt2)12g(tt2)2

At point B,

yB=lsinθ+(v2cosθ)(tBt2)12g(tBt2)2

According to given information,

v2=64.4sinθ(tBt2)=2cosθ0.3v2sinθyB=2sinθ+(v2cosθ)(tBt2)16.1(tBt2)2

For θ

Try θ=30°

v2=64.4sin30°=5.6745ft/s(tBt2)=2cos30°0.35.6745sin30°=0.50473syB=2sin30°+(5.6745cos30°)(0.50473)16.1(0.50473)2=0.62116ft

Try θ=45°

v2=64.4sin45°=6.7482ft/s(tBt2)=2cos45°0.36.7482sin30°=0.23351syB=2sin45°+(6.7482cos45°)(0.23351)16.1(0.23351)2=1.65060ft

Try θ=37.5°

v2=64.4sin37.5°=6.2613ft/s(tBt2)=2cos45°0.36.2613sin30°=0.33757syB=2sin45°+(6.2613cos45°)(0.33757)16.1(0.33757)2=1.05972ft

Then,

Let, u=θ30°

Therefore,

(u,yB)=(0°,0.62114 ft), (7.5°,1.05972 ft), (15°,1.65060 ft)

Therefore the quadratic curve equation will be,

yB=0.62114+0.29678u0.009688711u2

But, yB=0.4 ft

Therefore, above equation becomes,

0.009688711u2+0.29678u1.02114=0

By solving we get,

u=3.95° u=26.68°

Rejecting the second value, we get,

θ=30°+u=33.95°

Now, try θ=33.95°

v2=64.4sin33.95°=5.997ft/s(tBt2)=2cos33.95°0.35.997sin33.95°=0.40578syB=2sin33.95°+(5.997cos33.95°)(0.40578)16.1(0.40578)2=0.48462f

Therefore, new quadratic curve fits,

(u,yB)=(0°,0.62114 ft), (3.95°, 0.48462 ft), (7.5°,1.05972)

Then the quadratic equation will be,

yB=0.62114+0.342053907u0.015725232u2

But, yB=0.4 ft

Therefore, above equation becomes,

0.015725232u2+0.342053907u1.02114=0

Solve to find u

u=3.572°

Then,

θ=30°+3.572°=33.572°

Now, try θ=33.572°

v2=64.4sin33.572°=5.9676ft/s(tBt2)=2cos33.572°0.35.9676sin33.572°=0.41406syB=2sin33.572°+(5.9676cos33.572°)(0.41406)16.1(0.41406)2=0.40445ft

Above value of yB is close enough to 0.4 ft

Now substitute θ=33.572° And v2=5.9676ft/s

Therefore,

v02=v22+2gl(1+sinθ)v02=(5.9676ft/s)2+2(9.81m/s2)(2)(1+sin33.572°)v0=15.35ft/s

Conclusion:

The initial velocity is equal to v0=15.35ft/s

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Chapter 13 Solutions

Vector Mechanics For Engineers

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